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Revision 1.2 by greg, Thu May 26 18:53:04 2005 UTC vs.
Revision 1.17 by greg, Sat Nov 17 01:13:50 2007 UTC

# Line 1 | Line 1
1   .\" RCSid "$Id$"
2 < .TH RPIECE 1 5/25/05 RADIANCE
2 > .TH RTCONTRIB 1 5/25/05 RADIANCE
3   .SH NAME
4 < rtcontrib - compute contributions in a RADIANCE scene
4 > rtcontrib - compute contribution coefficients in a RADIANCE scene
5   .SH SYNOPSIS
6   .B rtcontrib
7   [
8   .B "\-n nprocs"
9   ][
10 + .B \-V
11 + ][
12 + .B \-c
13 + ][
14 + .B \-fo
15 + |
16 + .B \-r
17 + ][
18   .B "\-e expr"
19   ][
20   .B "\-f source"
21   ][
22 < .B "\-o fspec"
22 > .B "\-o ospec"
23   ][
24   .B "\-b binv"
25 + ][
26 + .B "\-bn nbins"
27   ]
28 < .B "\-m mod .."
28 > {
29 > .B "\-m mod | \-M file"
30 > }
31 > ..
32   [
33   .B $EVAR
34   ]
# Line 26 | Line 39 | rtcontrib - compute contributions in a RADIANCE scene
39   rtrace options
40   ]
41   .B octree
42 + .br
43 + .B "rtcontrib [ options ] \-defaults"
44   .SH DESCRIPTION
45   .I Rtcontrib
46 < computes ray contributions (i.e., color coefficients)
46 > computes ray coefficients
47   for objects whose modifiers are named in one or more
48   .I \-m
49   settings.
50   These modifiers are usually materials associated with
51   light sources or sky domes, and must directly modify some geometric
52   primitives to be considered in the output.
53 < The computed contributions can then be used in linear combination to
53 > A modifier list may also be read from a file using the
54 > .I \-M
55 > option.
56 > The RAYPATH environment variable determines directories to search for
57 > this file.
58 > (No search takes place if a file name begins with a '.', '/' or '~'
59 > character.)\0
60 > .PP
61 > By setting the boolean
62 > .I \-V
63 > option, you may instruct
64 > .I rtcontrib
65 > to report the contribution from each material rather than the ray
66 > coefficient.
67 > This is particularly useful for light sources with directional output
68 > distributions, whose value would otherwise be lost in the shuffle.
69 > With the default
70 > .I -V-
71 > setting, the output of rtcontrib is a coefficient that must be multiplied
72 > by the radiance of each material to arrive at a final contribution.
73 > This is more convenient for computing daylight coefficeints, or cases
74 > where the actual radiance is not desired.
75 > Use the
76 > .I -V+
77 > setting when you wish to simply sum together contributions
78 > (with possible adjustment factors) to obtain a final radiance value.
79 > Combined with the
80 > .I \-i
81 > or
82 > .I \-I
83 > option, irradiance contributions are reported by
84 > .I \-V+
85 > rather than radiance, and
86 > .I \-V-
87 > coefficients contain an additonal factor of PI.
88 > .PP
89 > The output of
90 > .I rtcontrib
91 > has many potential uses.
92 > Source contributions can be used as components in linear combination to
93   reproduce any desired variation, e.g., simulating lighting controls or
94   changing sky conditions via daylight coefficients.
95   More generally,
96   .I rtcontrib
97 < may be used to compute input-output relationships in optical
98 < systems, such as light pipes and shading devices.
97 > can be used to compute arbitrary input-output relationships in optical
98 > systems, such as luminaires, light pipes, and shading devices.
99   .PP
100 + Setting the
101 + .I \-c
102 + option instructs
103 + .I rtcontrib
104 + to accumulate values rather than reporting one record per ray.
105 + With this option, only a single record will be produced at the very
106 + end, corresponding to the sum of all rays given on the input.
107 + This is equivalent to passing all the output records through a program like
108 + .I total(1)
109 + to sum RGB values together, but is much more efficient.
110 + Using this option, it is possible to reverse sampling, sending rays from
111 + a parallel source such as the sun to a diffuse surface, for example.
112 + Care must be taken to perform normalization based on the
113 + radiation density and the number of rays sampled.
114 + .PP
115   .I Rtcontrib
116   calls
117   .I rtrace(1)
118 < to calculate the contributions for each input ray,
119 < and the output tallies are sent to one or more files according to the
118 > with the \-oTW (or \-oTV) option to calculate the daughter ray
119 > contributions for each input ray, and the output tallies
120 > are sent to one or more destinations according to the given
121   .I \-o
122   specification.
123 + If a destination begins with an exclamation mark ('!'), then
124 + a pipe is opened to a command and data is sent to its standard input.
125 + Otherwise, the destination is treated as a file.
126 + An existing file of the same name will not be clobbered, unless the
127 + .I \-fo
128 + option is given.
129 + If instead the
130 + .I \-r
131 + option is specified, data recovery is attempted on existing files.
132 + (If
133 + .I \-c
134 + is used together with the
135 + .I \-r
136 + option, existing files are read in and new ray evaluations are added
137 + to the previous results, providing a convenient means for
138 + progressive simulation.)\0
139   If an output specification contains a "%s" format, this will be
140   replaced by the modifier name.
141   The
# Line 58 | Line 144 | option may be used to further define
144   a "bin number" within each object if finer resolution is needed, and
145   this will be applied to a "%d" format in the output file
146   specification if present.
147 < (The actual bin number is computed at run time based on ray direction
148 < and surface intersection, as described below.)\0
147 > The actual bin number is computed at run time based on ray direction
148 > and surface intersection, as described below.
149 > If the number of bins is known in advance, it should be specified with the
150 > .I \-bn
151 > option, and this is critical for output files containing multiple values
152 > per record.
153 > Since bin numbers start from 0, the bin count is always equal to
154 > the last bin plus 1.
155 > Set the this value to 0 if the bin count is unknown (the default).
156   The most recent
157 < .I \-b
157 > .I \-b,
158 > .I \-bn
159   and
160   .I \-o
161   options to the left of each
162   .I \-m
163   setting affect only that modifier.
164 < (The ordering of other options is unimportant.)\0
164 > The ordering of other options is unimportant, except for
165 > .I \-x
166 > and
167 > .I \-y
168 > if the
169 > .I \-c
170 > is present, when they control the resolution string
171 > produced in the corresponding output.
172   .PP
173   If a
174   .I \-b
# Line 80 | Line 181 | the variables Px, Py, and Pz, and the normalized ray d
181   will be assigned to Dx, Dy, and Dz.
182   These parameters may be combined with definitions given in
183   .I \-e
184 < options and files read in
184 > arguments and files read using the
185   .I \-f
186 < options, to compute the bin, which will be
186 > option.
187 > The computed bin value will be
188   rounded to the nearest whole number.
189   This mechanism allows the user to define precise regions or directions
190   they wish to accumulate, such as the Tregenza sky discretization,
191   which would be otherwise impossible to specify
192   as a set of RADIANCE primitives.
193 + The rules and predefined functions available for these expressions are
194 + described in the
195 + .I rcalc(1)
196 + man page.
197 + Unlike
198 + .I rcalc,
199 + .I rtcontrib
200 + will search the RADIANCE library directories for each file given in a
201 + .I \-f
202 + option.
203   .PP
204   If no
205   .I \-o
206   specification is given, results are written on the standard output in order
207   of modifier (as given on the command line) then bin number.
208 < Concatenated data is also sent to a lone output file (i.e., an initial
208 > Concatenated data is also sent to a single destination (i.e., an initial
209   .I \-o
210   specification without formatting strings).
211   If a "%s" format appears but no "%d" in the
# Line 152 | Line 264 | replaced by the contents of the given file.
264   To compute the proportional contributions from sources modified
265   by "light1" vs. "light2" on a set of illuminance values:
266   .IP "" .2i
267 < rtcontrib -I+ @render.opt -o c_%s.dat -m light1 -m light2 scene.oct < test.dat
267 > rtcontrib \-I+ @render.opt \-o c_%s.dat \-m light1 \-m light2 scene.oct < test.dat
268   .PP
269   To generate a pair of images corresponding to these two lights'
270   contributions:
271   .IP "" .2i
272 < vwrays -ff -x 1024 -y 1024 -vf best.vf |
273 < rtcontrib -ffc `vwrays -d -x 1024 -y 1024 -vf best.vf`
274 < @render.opt -o c_%s.pic -m light1 -m light2 scene.oct
272 > vwrays \-ff \-x 1024 \-y 1024 \-vf best.vf |
273 > rtcontrib \-ffc `vwrays \-d \-x 1024 \-y 1024 \-vf best.vf`
274 > @render.opt \-o c_%s.pic \-m light1 \-m light2 scene.oct
275   .PP
276   These images may then be recombined using the desired outputs
277   of light1 and light2:
278   .IP "" .2i
279 < pcomb -c 100 90 75 c_light1.pic -c 50 55 57 c_light2.pic > combined.pic
279 > pcomb \-c 100 90 75 c_light1.pic \-c 50 55 57 c_light2.pic > combined.pic
280   .PP
281   To compute an array of illuminance contributions according to a Tregenza sky:
282   .IP "" .2i
283 < rtcontrib -b tbin -o sky.dat -m skyglow -b 0 -o ground.dat -m groundglow
284 < @render.opt -f tregenza.cal scene.oct < test.dat
283 > rtcontrib \-I+ \-b tbin \-o sky.dat \-m skyglow \-b 0 \-o ground.dat \-m groundglow
284 > @render.opt \-f tregenza.cal scene.oct < test.dat
285 > .SH ENVIRONMENT
286 > RAYPATH         path to search for \-f and \-M files
287   .SH AUTHOR
288   Greg Ward
289   .SH "SEE ALSO"
290   cnt(1), getinfo(1), pcomb(1), pfilt(1), ra_rgbe(1),
291 < rcalc(1), rpict(1), rtrace(1), vwrays(1), ximage(1)
291 > rcalc(1), rpict(1), rtrace(1), total(1), vwrays(1), ximage(1)

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